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Spectral Fukaya Category Overview

Updated 12 July 2026
  • Spectral Fukaya category is a framework that refines traditional Fukaya theory by incorporating additional homotopical, monodromic, or eigenvalue data.
  • It encompasses enrichment over spectra, eigenvalue decomposition of quantum cohomology, and deformation-theoretic enhancements using B-fields and divisor data.
  • Applications include advances in mirror symmetry, Weinstein localization, and computational approaches via sheaf-theoretic methods and homotopy colimits.

Spectral Fukaya category denotes a family of related refinements of Fukaya-theoretic constructions rather than a single universally fixed object. In the cited literature, the phrase is used for at least four closely connected patterns: a Fukaya category enriched over bordism groups or spectra; a decomposition of a Fukaya category into summands indexed by the spectrum of quantum multiplication or by critical values of a Landau–Ginzburg potential; a sheaf of stable \infty-categories on a Weinstein manifold; and a deformation-theoretic package in which AA_\infty-operations vary under BB-fields, divisor data, or symplectic-cohomological Maurer–Cartan elements. This suggests that “spectral Fukaya category” functions as an umbrella term for stable-homotopical, monodromic, or eigenvalue-sensitive enhancements of Fukaya categories (Porcelli et al., 25 Sep 2025, Castronovo, 2018, Nadler, 2011, Rabah, 3 Jul 2026).

1. Terminological scope

The cited literature uses “spectral” in several technically distinct senses. Some papers mean an actual enrichment over spectra or bordism theories. Others mean a spectral decomposition by eigenvalues of c1c_1\star or of a mirror superpotential. Others use “spectral” for categorical sheaf-theoretic localization or for stability data encoded by spectral networks. The common feature is that the Fukaya category is no longer treated as only an abstract chain-level AA_\infty-category over a field; it is organized by additional homotopical, monodromic, or eigenvalue data.

Usage Core datum Representative source
Spectrum or bordism enrichment Thom spectrum RΨR_\Psi, morphisms ΩEΨ(MLK)\Omega_*^{E_\Psi}(M^{LK}) (Porcelli et al., 25 Sep 2025)
Eigenvalue decomposition Summands Fλ(X)\mathcal F_\lambda(X), QH(X)=λQHλ(X)QH^*(X)=\bigoplus_\lambda QH_\lambda(X) (Castronovo, 2018, Smith, 2018)
Sheaf of stable categories FΛ\mathcal F_\Lambda on the conic topology, AA_\infty0 (Nadler, 2011)
Deformation-theoretic refinement AA_\infty1-field twisting, relative divisor variables AA_\infty2, Maurer–Cartan deformation (Azam et al., 2023, Rabah, 3 Jul 2026)

A recurrent misconception is that “spectral Fukaya category” always means enrichment over spectra in the strict homotopy-theoretic sense. The literature shows a broader usage. In toric and Grassmannian contexts, “spectral” can instead mean decomposition into generalized eigensummands of quantum cohomology; in Weinstein localization, it can mean a sheaf of stable categories; and in exact bordism-theoretic work it can mean an honest spectrum-level or Thom-spectrum-valued refinement (Castronovo, 2018, Nadler, 2011, Porcelli et al., 25 Sep 2025).

2. Spectrum-enriched and bordism-theoretic constructions

The most literal realization of the term appears in work on exact Liouville domains equipped with tangential data AA_\infty3. There one constructs a spectral Fukaya category AA_\infty4 whenever AA_\infty5 lifts to AA_\infty6, with objects AA_\infty7 consisting of closed exact Lagrangians endowed with compatible AA_\infty8-orientations. Morphisms are not Floer cochain complexes over a ring; they are bordism groups of AA_\infty9-oriented flow modules over Floer flow categories,

BB0

where BB1 is a Thom BB2-monoid and BB3 is the associated commutative ring spectrum with bordism theory BB4 (Porcelli et al., 25 Sep 2025).

In this model, tangential data are fundamental. The homotopy fibre of BB5 determines a Thom BB6-monoid, and Bott periodicity and index theory produce the ring spectrum BB7. The resulting category is “spectral” in a strong sense: its enrichment is controlled by a Thom spectrum rather than by ordinary coefficients. Classical examples occur when BB8, giving the sphere spectrum and framed bordism, or when BB9, giving c1c_1\star0 and complex cobordism (Porcelli et al., 25 Sep 2025).

This framework also incorporates rank-one spectral local systems. A rank-one spectral local system is a map

c1c_1\star1

the spectral analogue of a rank-one local system of modules. Twisting by c1c_1\star2 modifies the flow categories and yields a local-system-enriched spectral Fukaya category. The associated open-closed class satisfies the explicit formula

c1c_1\star3

where c1c_1\star4 is a multiplicatively two-torsion unit arising from the action of the stable Hopf map c1c_1\star5. In contrast to classical exact Fukaya categories over c1c_1\star6, where the open-closed image of a brane is independent of the rank-one local system, the spectral local system contributes a nontrivial c1c_1\star7-primary correction (Porcelli et al., 25 Sep 2025).

This construction supplies a precise bordism-theoretic enhancement of exact Fukaya theory. It is also a template for how stable homotopy data can enter Fukaya categories without passing through a purely algebraic dg model first.

3. Spectral decomposition by quantum cohomology and mirror superpotentials

A second major meaning of “spectral Fukaya category” is decomposition into summands indexed by the spectrum of quantum multiplication. In the monotone setting one decomposes

c1c_1\star8

where c1c_1\star9 is the generalized eigenspace for AA_\infty0 with eigenvalue AA_\infty1. Correspondingly, one defines Fukaya summands AA_\infty2 whose objects satisfy AA_\infty3, so that

AA_\infty4

In this usage, the spectral Fukaya category is the collection of these eigensummands and their mirror identification with fibres AA_\infty5 of a Landau–Ginzburg superpotential AA_\infty6 (Castronovo, 2018).

The Grassmannian case makes this formulation explicit. For AA_\infty7, the eigenvalues of AA_\infty8 are

AA_\infty9

where RΨR_\Psi0 runs over size-RΨR_\Psi1 subsets of roots of RΨR_\Psi2. The paper identifies the monotone Gelfand–Cetlin torus RΨR_\Psi3, computes its Maslov RΨR_\Psi4 disk potential, and shows that its holonomy local systems provide nonzero objects in the corresponding spectral summands. For RΨR_\Psi5 with RΨR_\Psi6 prime, all eigenvalues have multiplicity one, which yields a complete set of generators for all spectral summands and a fibrewise homological mirror symmetry statement

RΨR_\Psi7

for every eigenvalue RΨR_\Psi8 (Castronovo, 2018).

In compact toric varieties, the same pattern is organized through the decomposition

RΨR_\Psi9

with each summand ΩEΨ(MLK)\Omega_*^{E_\Psi}(M^{LK})0 associated to a toric fibre ΩEΨ(MLK)\Omega_*^{E_\Psi}(M^{LK})1 equipped with a rank ΩEΨ(MLK)\Omega_*^{E_\Psi}(M^{LK})2 local system. The closed-open string map factors through the Kodaira–Spencer isomorphism on each summand, and, assuming an appropriate version of Abouzaid’s criterion, ΩEΨ(MLK)\Omega_*^{E_\Psi}(M^{LK})3 split-generates the corresponding summand of the Fukaya category (Smith, 2018). Here “spectral” refers not to stable homotopy types but to the spectrum of the quantum cohomology algebra and to the mirror critical-point decomposition of the Jacobian ring.

This eigenvalue-based usage is now standard in monotone mirror symmetry. It aligns Fukaya-theoretic decomposition with the decomposition of the mirror Landau–Ginzburg model into critical-value fibres, thereby turning the spectral data of ΩEΨ(MLK)\Omega_*^{E_\Psi}(M^{LK})4 into a categorical direct-sum structure.

4. Twists, deformations, and open–closed structures

A third cluster of meanings concerns controlled deformations of Fukaya categories. One source is ΩEΨ(MLK)\Omega_*^{E_\Psi}(M^{LK})5-field twisting. For a symplectic manifold ΩEΨ(MLK)\Omega_*^{E_\Psi}(M^{LK})6 with closed ΩEΨ(MLK)\Omega_*^{E_\Psi}(M^{LK})7-form ΩEΨ(MLK)\Omega_*^{E_\Psi}(M^{LK})8, the relevant complexified symplectic form is

ΩEΨ(MLK)\Omega_*^{E_\Psi}(M^{LK})9

Objects are Lagrangian branes Fλ(X)\mathcal F_\lambda(X)0 such that

Fλ(X)\mathcal F_\lambda(X)1

Morphisms are Floer complexes with coefficients in fibrewise homomorphisms of the line bundles, and the Fλ(X)\mathcal F_\lambda(X)2-operations are weighted by

Fλ(X)\mathcal F_\lambda(X)3

together with parallel transport along the boundary segments. The weight depends only on the homotopy class of the disk, and under a Lagrangian isotopy Fλ(X)\mathcal F_\lambda(X)4 it changes by

Fλ(X)\mathcal F_\lambda(X)5

Exact isotopies give trivial factors, while non-exact isotopies produce controlled twists by classes in Fλ(X)\mathcal F_\lambda(X)6 (Azam et al., 2023).

This Fλ(X)\mathcal F_\lambda(X)7-field formalism is not yet a spectrum-enriched category, but it supplies precisely the homotopy-invariant twisting and isotopy-control that a stable or parameterized refinement would require. The paper itself presents these ingredients as what one needs to think about “spectral Fukaya categories”: stable homotopy refinements, spectral enrichments, and twisted or parameterized variants (Azam et al., 2023).

A second deformation-theoretic source is the relative Fukaya category. For a closed monotone symplectic manifold Fλ(X)\mathcal F_\lambda(X)8 with simple normal-crossings divisor Fλ(X)\mathcal F_\lambda(X)9, one defines

QH(X)=λQHλ(X)QH^*(X)=\bigoplus_\lambda QH_\lambda(X)0

and constructs a relative Fukaya category QH(X)=λQHλ(X)QH^*(X)=\bigoplus_\lambda QH_\lambda(X)1 whose objects are the same compact exact branes as those of QH(X)=λQHλ(X)QH^*(X)=\bigoplus_\lambda QH_\lambda(X)2, QH(X)=λQHλ(X)QH^*(X)=\bigoplus_\lambda QH_\lambda(X)3, but whose QH(X)=λQHλ(X)QH^*(X)=\bigoplus_\lambda QH_\lambda(X)4-operations record intersection multiplicities with QH(X)=λQHλ(X)QH^*(X)=\bigoplus_\lambda QH_\lambda(X)5 through monomials QH(X)=λQHλ(X)QH^*(X)=\bigoplus_\lambda QH_\lambda(X)6. The associated deformation on the wrapped side is governed by a Maurer–Cartan element

QH(X)=λQHλ(X)QH^*(X)=\bigoplus_\lambda QH_\lambda(X)7

in an QH(X)=λQHλ(X)QH^*(X)=\bigoplus_\lambda QH_\lambda(X)8-algebra built from symplectic cohomology, and the closed–open QH(X)=λQHλ(X)QH^*(X)=\bigoplus_\lambda QH_\lambda(X)9-morphism transfers FΛ\mathcal F_\Lambda0 to Hochschild cochains of the wrapped category. The main theorem identifies the resulting deformed wrapped category on compact objects with the relative Fukaya category, proving Conjecture FΛ\mathcal F_\Lambda1 of SBEAS24.

Open–closed maps supply the algebraic backbone for these deformation pictures. In the wrapped exact setting, one has a map from Hochschild homology to symplectic cohomology, and if the identity FΛ\mathcal F_\Lambda2 lies in its image for a full subcategory, then that subcategory split-generates the wrapped Fukaya category (Abouzaid, 2010). This gives a precise mechanism by which closed-string “spectral” data control open-string generation.

Taken together, these constructions show that spectral Fukaya theory can also mean a deformation package: FΛ\mathcal F_\Lambda3-field phases, divisor variables, Maurer–Cartan elements in symplectic cohomology, and closed–open transfer to Hochschild cochains.

5. Local-to-global, sheaf-theoretic, and homotopy-colimit formulations

A fourth meaning of “spectral Fukaya category” is local-to-global organization by stable or dg-categorical descent. In Nadler’s categorical Morse-theoretic formulation for Weinstein manifolds, the perfect Fukaya category is not treated as a single indivisible object. Instead, one associates local Fukaya categories to Weinstein cells and glues them by recollement. For a marked Weinstein manifold FΛ\mathcal F_\Lambda4, one obtains a sheaf FΛ\mathcal F_\Lambda5 of stable FΛ\mathcal F_\Lambda6-linear FΛ\mathcal F_\Lambda7-categories on the conic topology of FΛ\mathcal F_\Lambda8, supported on the characteristic cone FΛ\mathcal F_\Lambda9, with

AA_\infty00

Locally above each unstable cell AA_\infty01, the sheaf restricts to a category equivalent to AA_\infty02, where AA_\infty03 is the Weinstein cell obtained by Hamiltonian reduction (Nadler, 2011).

This is “spectral” in the sense of higher-categorical localization. The Fukaya category becomes the global sections of a sheaf of stable AA_\infty04-categories, and cell-wise recollement behaves as a categorified Morse decomposition. The paper also suggests a dual cosheaf picture for partially wrapped categories, further reinforcing the local-to-global interpretation (Nadler, 2011).

A more computational dg-categorical realization appears in work on homotopy colimits. For semifree dg categories, one constructs an explicit cylinder object and an explicit formula for homotopy colimits in AA_\infty05. Combined with the sectorial descent theorem of Ganatra–Pardon–Shende, this gives practical formulas computing wrapped Fukaya categories of Weinstein manifolds from sectorial coverings. In particular, wrapped Fukaya categories of cotangent bundles and plumbing spaces can be computed by dg homotopy colimits, and for lens spaces the endomorphism algebra of the cotangent fibre detects the homotopy type (Karabas et al., 2021).

The sheaf-theoretic realization of Fukaya categories at infinity provides another nearby development. For Legendrian knots in the contact boundary of a cotangent bundle, the relevant Fukaya category is equivalent to a dg category of constructible sheaves with singular support controlled by the front projection. In positive braid situations, weight filtrations on pushforwards from moduli spaces of such objects produce spectral sequences whose AA_\infty06-page is colored triply graded Khovanov–Rozansky homology (Shende et al., 2014). This does not use “spectral Fukaya category” in the same way as spectrum enrichment, but it shows how categorical localization can produce genuinely spectral invariants.

These local-to-global pictures replace a single chain complex by stable gluing data, recollement, and homotopy colimits. In that sense they are among the most structurally “spectral” approaches in the current literature.

6. Monodromy, stability conditions, and adjacent programs

Lefschetz fibrations provide another source of spectral structure. For the directed Fukaya algebra AA_\infty07 of vanishing thimbles in an exact symplectic Lefschetz fibration, the monodromy around infinity AA_\infty08 yields a canonical map

AA_\infty09

so classes in fixed-point Floer cohomology produce natural transformations from the Serre functor to the identity. In the anticanonical pencil case, one obtains a distinguished pair AA_\infty10 of bimodule maps AA_\infty11, and these are organized by Seidel into the framework of noncommutative divisors and pencils (Seidel, 2014). Here “spectral” refers to monodromy data, Serre functor sections, and the family of categorical structures parametrized by the pencil.

A different adjacent program appears in Fukaya categories with coefficients. Given a surface, a triangulated dg-category AA_\infty12, and a holomorphic family of Bridgeland stability conditions on AA_\infty13, one defines spectral networks as objects in a Fukaya category of the surface with coefficients in AA_\infty14. In the constant-family case, a spectral network of phase AA_\infty15 is a graph-supported object whose fibre labels are semistable and whose total phase is constant; its central charge is

AA_\infty16

The paper conjectures that semistable objects of the resulting Fukaya category with coefficients are precisely those admitting spectral network representatives, proves a uniqueness theorem up to AA_\infty17-equivalence of the fibre data, and verifies the conjecture for a disk with six marked boundary points and coefficient category AA_\infty18 (Haiden et al., 2021).

These programs clarify why the term remains nonuniform. “Spectral Fukaya category” may denote a bordism-enriched category, an eigenvalue decomposition, a monodromy-controlled Lefschetz-theoretic structure, or a stability-theoretic surface category with spectral-network representatives. The cited literature therefore supports a cautious encyclopedia definition: the phrase refers to a family of constructions in which Fukaya categories are refined by spectra, by spectral decompositions, by sheaf-theoretic localization, or by deformation and stability data, with mirror symmetry providing the principal unifying context (Porcelli et al., 25 Sep 2025, Castronovo, 2018, Seidel, 2014, Haiden et al., 2021).

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